Fermi level pinning effect Fermi level pinning is a hot spot in the field of semiconductor science and technology. The Fermi level pinning effect is an important concept in semiconductor physics. Originally, the Fermi level in semiconductors is prone to position changes. For example, doping the donor impurity can move the Fermi energy level to the bottom of the conduction band, and the semiconductor becomes an n-type semiconductor; doping the acceptor impurity can make the Fermi energy level move to the top of the valence band, and the semiconductor becomes a p-type semiconductor. However, if the position of the Fermi level cannot change due to doping, etc., then this situation is called the Fermi level pinning effect. When this effect works, even if a lot of donors or acceptors are doped into the semiconductor, they cannot be activated (that is, they cannot provide carriers), so the type of the semiconductor cannot be changed, so it is difficult to make it through impurity compensation. Out of the pn junction. The reason for the Fermi level pinning effect is related to the nature of the material. Wide bandgap semiconductors ( GaN , SiC , etc.) are a typical example. Generally, such semiconductors can only be prepared as n-type or p-type semiconductors, and their type cannot be changed by doping (that is, the Fermi energy level cannot be moved), so it is called Unipolar semiconductor. Generally, semiconductors with strong ionic properties (such as II-VI semiconductors, CdS , ZnO , ZnSe , CdSe ) are often unipolar semiconductors. This is mainly due to the existence of a large number of charged defects, which make the Fermi level pinned. Because of this, when GaN is used to make blue-emitting diodes, it has previously encountered great difficulties. Later, the doped donor or acceptor impurities were activated through special annealing measures, and a pn junction was obtained—— Diodes that emit blue light. Amorphous semiconductors also often have Fermi level pinning effects. Most of the produced amorphous semiconductors are high-resistance materials, and the Fermi energy level cannot be moved due to doping, which is also due to the large number of defects in it.